Electromagnetic piezoelectric acoustic sensor

a piezoelectric acoustic sensor and piezoelectric technology, applied in the direction of mechanical audible signalling, solid analysis using sonic/ultrasonic/infrasonic waves, magnetic measurement, etc., can solve the problem of reducing sensitivity and interpretation complications, wave penetration still overshoots interfacial chemistry with loss of sensitivity, and provides a sufficiently compact evanescent zone to fully recover biochemical signals

Inactive Publication Date: 2010-08-10
STEVENSON ADRIAN +1
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  • Summary
  • Abstract
  • Description
  • Claims
  • Application Information

AI Technical Summary

Problems solved by technology

However there are significant problems with these systems.
An evanescent sensing region that is significantly thicker than the chemical layer of interest leads to reduced sensitivity and interpretation complications.
Focusing the evanescent wave towards the interface has been attempted with magnetic acoustic resonance sensors that work at 50 MHz, however wave penetration still overshoots the interfacial chemistry with losses in sensitivity.
Surface acoustic wave devices known as the Love wave device can work at higher frequencies for smaller penetration depths, however none of these systems provide a sufficiently compact evanescent zone to fully recover the biochemical signal.
A further restriction of these sensors is that a very limited window of information is recovered, at a single wavelength or frequency.
This is tantamount to operating an IR spectrometer at a single wavelength, which severely reduces the value of the data recovered.
With respect to the practical format of these systems, all optical and acoustic devices require additional layers of metallisation to be applied and patterned, which for the interdigitated pattern on SAW (surface acoustic wave) is an especially costly process.
Wire connections to QSM and SAW devices are required, which reduces compatibility with chemical immobilisation modifications and procedures and places design constraints on commercial instruments.

Method used

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Examples

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Embodiment Construction

[0031]FIG. 1b and FIG. 2 show an example arrangement in a sensor according to the present invention. A coil 1 receives RF current 4 via a multiply resonant transmission line 6. The electromagnetic field 5 produced by the coil 1 drives a piezoelectric element 3 to produce acoustic waves by electrostriction. The sensing done by the acoustic waves occurs either directly or indirectly. The substance to be detected either adsorbs to the vibrating surface, or a receptor can be attached to the vibrating surface, which is specific to the substance to be detected. When the substance adsorbs, it changes the acoustic spectrum. The coil 1 also acts as a detector which converts the changed electromagnetic field caused by the changed acoustic waves back into a RF current which is detected by a detection circuit, which includes an AM-diode detector 7 in this example.

[0032]The present invention eliminates the need for fine tuning between the transmission line 6 and the coil 1 in order to generate t...

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Abstract

An acoustic sensor comprises at least one resonant element. A driver comprises an electrical coupling means and an electromagnetic field source arranged such that the electrical coupling means transfers currents to the electromagnetic field source. The electromagnetic field source produces an electromagnetic field that drives the resonant elements to produce acoustic waves directed to a predetermined part of a test sample. Also provided is an electromagnetic detector for receiving the acoustic spectrum omitted from a test sample and an electrical circuit connected to the drive around detector.

Description

BACKGROUND OF THE INVENTION[0001]1. Field of the Invention[0002]Acoustic sensors which employ resonators have been used as detection devices for biological molecules for the past two decades, exhibiting sensitivity in the ng / ml range. They share with optical devices an ability to produce evanescent waves that propagate a limited distance across the solid liquid interface, so molecular events and processes in the bulk are not detected; only those processes leading to interfacial elasticity, viscosity, viscoelasticity and slippage are detected.[0003]2. The Prior Art[0004]However there are significant problems with these systems. As the dimensions of the molecules of interest range from 5 to 20 nm, a substantial amount (>95%) of acoustic transverse coupling is to the fluid above the chemical interface, essentially outside of the domain of the analysis in which there is interest.[0005]An evanescent sensing region that is significantly thicker than the chemical layer of interest leads...

Claims

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Application Information

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Patent Type & Authority Patents(United States)
IPC IPC(8): G01R33/20G01N27/72G01N27/00
CPCG01N29/036G01N2291/014G01N2291/0256G01N2291/101
Inventor STEVENSON, ADRIANLOWE, CHRISTOPHER ROBIN
Owner STEVENSON ADRIAN
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